LED Intensity Decay Particle Tracking Velocimetry (PTV)

Instrumentation
LED Intensity Decay Particle Tracking Velocimetry (PTV) (LAR-TOPS-394)
A cost-effective, high-resolution alternative to laser-based PTV systems
Overview
Particle tracking velocimetry (PTV) is a common technique used for measuring fluid flow by tracking the motion of small, micron-sized particles seeded in a fluid medium. Traditionally, PTV and its related technique, particle image velocimetry (PIV), rely on high-powered pulsed lasers that generate thin, intense light sheets to illuminate the particles. A high-speed camera captures sequential images, and advanced processing algorithms determine velocity vectors based on the displacement of the particles over time. While effective, these laser-based systems require expensive components, precise optical setups, and complex synchronization between the laser pulses and the camera, making them costly and challenging to implement. Innovators at NASA’s Langley Research Center (LaRC) have developed LED Intensity Decay Particle Tracking Velocimetry (LED-ID PTV), an alternative to conventional PTV that uses light-emitting diodes (LEDs) for flow illumination. LED-ID PTV leverages the natural capacitive intensity decay of LEDs to encode velocity and directional information passively. This approach eliminates the need for expensive cameras capable of double-pulsing exposures, lasers, and intricate timing mechanisms while still delivering high-resolution flow field data. The system is cost-effective, eye-safe, and adaptable to various experimental conditions, making it ideal for aerospace, industrial, and research applications.

The Technology
NASA’s LED-ID PTV system illuminates a seeded flow with an LED rather than a laser. Instead of using double-pulsed laser flashes to capture two separate images of particle positions, the system relies on the inherent intensity decay of an LED pulse to encode velocity information directly into a single long-exposure image. The LED’s light intensity decreases over time due to capacitor discharge characteristics of the driving circuit. This controlled decay serves as a built-in intensity marker, allowing for precise determination of particle velocity and directionality without requiring an actively modulated light source. In a single-color configuration, a monochrome camera captures a long- exposure image of particle streaks as they move through the illuminated region. Because the light intensity is continuously decreasing, the recorded streaks naturally encode velocity information based on their brightness gradient. Faster-moving particles create longer streaks, while slower particles form shorter ones. The intensity variation across the streak provides additional data about directionality, enabling flow field analysis with a minimal hardware setup. For more complex flow analysis, a two-color configuration can be employed to track three- dimensional motion. In this setup, two LEDs of different colors are positioned adjacent to each other to create overlapping light sheets. A color camera, or two monochrome cameras with a dichroic mirror, captures the streaks of particles as they move between these sheets. The color transition within a particle’s streak indicates its movement between the planes of illumination, allowing users to resolve out-of- plane velocity components. Image processing techniques (e.g., advanced algorithms, high-pass filtering methods, sub-interval streak segmentation) further enhance the system's accuracy. NASA’s LED-ID PTV system has been prototyped and demonstrated with excellent results, and is available for patent licensing to industry.
Schematic of the single-color LED-ID PTV system, where M is a small pick-of mirror to measure the intensity decay of each LED pulse. The camera images forward-scattered light from particles to maximize the intensity. Credit: NASA A schematic of the two-color LED-ID PTV system, where two monochrome cameras are used to increase imaging resolution/quality. Both cameras view the same scattering angle and field-of-view through the use of a dichroic mirror. Credit: NASA
Benefits
  • Cost-Effective: NASA’s LED-ID PTV system eliminates the need for expensive lasers and cameras capable of double-pulsing exposure. Equipment costs for a NASA prototype system were less than $1,000.
  • Improved Safety: Using LEDs in lieu of high powered, pulsed lasers reduces eye damage and electrocution risks.
  • 3D Flow Tracking Capabilities: By using two different color LEDs to illuminate adjacent or overlapping regions of the flow, NASA’s system can track not only in-plane (2D) velocity components, but also the out-of- plane velocity component - using only a single camera.
  • Provides Particle Direction Information: Conventional particle streak imaging shows the particle trace over a specified time duration, but the direction of the particle is unknown. Using NASA's LED-ID PTV, the direction of the particle motion is known (in the direction of decreasing intensity).
  • Simplified Imaging Setup: LED-ID PTV requires only an LED with its driving circuit and a standard camera.
  • Adaptable to Different Flow Speeds: Circuit capacitance can be changed to tailor the decay rate for different particle velocity ranges.
  • Flexible experimental configurations: LED-ID PTV works with single- or dual-camera setups, depending on imaging needs.

Applications
  • Aerospace: Measuring velocity fields in aerodynamic experiments such as wind tunnel testing.
  • Biomedical Flow Studies: Visualizing fluid flow in microfluidic and biological applications.
  • Industrial Fluid Dynamics: Assessing airflow in HVAC, combustion systems, and chemical reactors.
  • Environmental Studies: Analyzing air or water flow in atmospheric or hydrological research.
  • Automotive Aerodynamics: Investigating airflow over vehicles for fuel efficiency improvements.
  • Educational and Research Labs: Providing a cost-effective alternative for flow visualization experiments.
Technology Details

Instrumentation
LAR-TOPS-394
LAR-20413-1
Patent Pending
“LED Intensity Decay Particle Tracking Velocimetry,” Joshua M. Weisberger and Brett F. Bathel, NASA Langley Research Center, 07/2024, https://ntrs.nasa.gov/citations/20240007419
Similar Results
Simultaneous imaging system concept. On the left, particles and flow are visible when LCD grid-altered light is sampled. On the right only particles are visible when LCD-unaltered light is sampled.
Digital Projection Focusing Schlieren System
NASA’s digital projection focusing Schlieren system is attached to a commercial-off-the-shelf camera. For focusing Schlieren measurements, it directs light from the light source through a condenser lens and linear polarizer towards a beam-splitter where linear, vertically-polarized component of light is reflected onto the optical axis of the instrument. The light passes through the patterned LCD element, a polarizing prism, and a quarter-wave plate prior to projection from the assembly as left- or right-circularly polarized light. The grid-patterned light (having passed through the LCD element) is directed past the density object onto a retroreflective background (RBG) that serves as the source grid. Upon reflection off the RBG, the polarization state of light is mirrored. It passes the density object a second time and is then reimaged by the system. Upon encountering the polarizing prism the second time, the light is slightly offset. This refracted light passes through the LCD element, now serving as the cutoff grid, for a second time before being imaged by the camera. The LCD element can be programmed to display a variety of grid patterns to enable sensitivity to different density gradients. The color properties of the LCD can be leveraged in combination with multiple colored light sources to enable simultaneous multi-color, multi-technique data collection. This system is ready for integration into commercial flow visualization and diagnostic equipment, offering manufacturers and research facilities an efficient, cost-effective solution for multi-technique imaging. The Schlieren system is currently available for patent licensing.
https://images.nasa.gov/details-ACD16-0013-013
Beam Crossing Optical System
The conventional approaches for measuring focused laser differential interferometry either use a single-point mechanism that cannot calculate velocity or a system that creates non-parallel beams in the testing zone, causing differences in time to travel between beams throughout the testing zone, adding a level of uncertainty to velocity measurements. For this technology, the inventors determined that the best approach is to use a method that ensures all laser beams propagating between the transmitter and receiver sides of the instrument are parallel to one another. This is done by crossing two orthogonally polarized beams at a Wollaston prism located just ahead of the field lens on the transmitter side of the FLDI. The polarization orientation of the two crossing beams must be at ±45 degrees to one another so that the Wollaston prism can further split the beams by a small angle (this gives the instrument its sensitivity to density fluctuations at each measurement point). The use of wedge prisms (that comprise the beam crossing system) to redirect the split beams such that they cross the optical axis minimizes any distortion imparted to the beams. This is in contrast to the use of a spherical focusing lens to redirect the split beams, which can impart undesirable distortions to the beams and affect the focusing properties of the FLDI instrument between its transmitter and receiver sides.
Figure 1. Projected BOS image of the air flow out of a compressed air can using a projected pattern of 0.2 mm dots on a speckled glass slide.
Projected Background-Oriented Schlieren Imaging
The Projected BOS imaging system provides a significant advancement over other BOS flow visualization techniques. Specifically, the present BOS imaging method removes the need for a physically patterned retroreflective background within the flow of interest and is therefore insensitive to the changing conditions due to the flow. For example, in a wind tunnel used for aerodynamics testing, there are vibrations and temperature changes that can affect the entire tunnel and anything inside it. Any patterned background within the wind tunnel will be subject to these changing conditions and those effects must be accounted for in the post-processing of the BOS image. This post-processing is not necessary in the Projected BOS process here. In the Projected BOS system, a pattern is projected onto a retroreflective background across the flow of interest. The imaged pattern in this configuration can be made physically (a pattern on a transparent slide) or can be digitally produced on an LCD screen. In this projection scheme, a reference image can be taken at the same time as the signal image, facilitating real-time BOS imaging and allowing the pattern to be changed or optimized during measurements. The Projected BOS imaging technology has been proven to work by visualizing the air flow out of a compressed air canister taken with this new system. The Projected BOS is available for patent licensing.
Credit: NASA
Filtered Ronchi Rulings for Enhanced Schlieren Imaging
The first optic is a 1D Ronchi ruling, where shortpass or longpass filters replace the traditional opaque lines in the grid pattern. The second optic is a 2D Ronchi ruling, where one set of lines is made from shortpass filters and the orthogonal set from longpass filters. By using two colors of light and a color camera in the focusing schlieren system (or a dichroic mirror with two monochrome cameras), the 1D optic enables simultaneous focusing schlieren and other co-linear techniques, while the 2D optic allows for the unambiguous measurement of two orthogonal density gradients in focusing schlieren images. Unlike standard optical filters, which typically cover an entire substrate, these Ronchi rulings feature alternating clear and filtered regions in structured 1D or 2D patterns. By leveraging color filtering and a color camera, the 1D ruling enables simultaneous focusing schlieren and complementary optical diagnostics, such as Particle Image Velocimetry (PIV), Pressure-Sensitive Paint (PSP), and Thermal-Sensitive Paint (TSP). The 2D ruling enables simultaneous and unambiguous measurement of two orthogonal density gradients, a capability not possible with conventional Ronchi rulings. This advancement significantly improves the accuracy and efficiency of schlieren-based flow measurements. The types of filters are not just limited to shortpass and longpass coatings, but could include notch, bandpass, and multiple-bandpass filter coatings as well. This design expands the utility of schlieren imaging in high-speed aerodynamics, combustion diagnostics, and other fluid dynamics applications. This Ronchi ruling methodology is at TRL 4 (component and/or breadboard validation in a lab environment) and is available for patent licensing.
Device prototype in use
Optical Head-Mounted Display System for Laser Safety Eyewear
The system combines laser goggles with an optical head-mounted display that displays a real-time video camera image of a laser beam. Users are able to visualize the laser beam while his/her eyes are protected. The system also allows for numerous additional features in the optical head mounted display such as digital zoom, overlays of additional information such as power meter data, Bluetooth wireless interface, digital overlays of beam location and others. The system is built on readily available components and can be used with existing laser eyewear. The software converts the color being observed to another color that transmits through the goggles. For example, if a red laser is being used and red-blocking glasses are worn, the software can convert red to blue, which is readily transmitted through the laser eyewear. Similarly, color video can be converted to black-and-white to transmit through the eyewear.
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